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9702 · 25.2

Stellar radii — practice questions

Practice and worked examples for 9702 Stellar radii. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

A star is observed to have a radiant flux of 1.50×109 W m21.50 \times 10^{-9} \text{ W m}^{-2} at Earth and is 100100 light-years away. Its peak emission wavelength is 450 nm450 \text{ nm}. Estimate the star's radius.

(Given: 1 light-year = 9.46×1015 m9.46 \times 10^{15} \text{ m}, Wien's constant = 2.9×103 m K2.9 \times 10^{-3} \text{ m K}, Stefan-Boltzmann constant = 5.67×108 W m2 K45.67 \times 10^{-8} \text{ W m}^{-2} \text{ K}^{-4})

Show solution outline
  1. Convert distance to metres: d=100 ly×9.46×1015 m/ly=9.46×1017 md = 100 \text{ ly} \times 9.46 \times 10^{15} \text{ m/ly} = 9.46 \times 10^{17} \text{ m}
  2. Calculate Luminosity (L) using the inverse square law for flux: L=F×4πd2L = F \times 4\pi d^2 L=(1.50×109 W m2)×4π(9.46×1017 m)2L = (1.50 \times 10^{-9} \text{ W m}^{-2}) \times 4\pi (9.46 \times 10^{17} \text{ m})^2 L=1.68×1028 WL = 1.68 \times 10^{28} \text{ W}
  3. Convert peak wavelength to metres and calculate Temperature (T) using Wien's Law: λmax=450 nm=450×109 mλ_{max} = 450 \text{ nm} = 450 \times 10^{-9} \text{ m} T=constantλmax=2.9×103 m K450×109 mT = \frac{\text{constant}}{λ_{max}} = \frac{2.9 \times 10^{-3} \text{ m K}}{450 \times 10^{-9} \text{ m}} T=6444 KT = 6444 \text{ K} (approx 6400 K6400 \text{ K})
  4. Calculate Radius (r) using the Stefan-Boltzmann Law: Rearrange L=4πr2σT4L = 4\pi r^2 \sigma T^4 to solve for r: r=L4πσT4r = \sqrt{\frac{L}{4\pi \sigma T^4}} r=1.68×1028 W4π(5.67×108 W m2 K4)(6444 K)4r = \sqrt{\frac{1.68 \times 10^{28} \text{ W}}{4\pi (5.67 \times 10^{-8} \text{ W m}^{-2} \text{ K}^{-4}) (6444 \text{ K})^4}} r=1.68×10284π(5.67×108)(1.73×1015)r = \sqrt{\frac{1.68 \times 10^{28}}{4\pi (5.67 \times 10^{-8}) (1.73 \times 10^{15})}} r=1.68×10281.23×109r = \sqrt{\frac{1.68 \times 10^{28}}{1.23 \times 10^9}} r=1.37×1019r = \sqrt{1.37 \times 10^{19}} r=3.70×109 mr = 3.70 \times 10^9 \text{ m}

The star's radius is approximately 3.70×109 m3.70 \times 10^9 \text{ m} (or 3.7×106 km3.7 \times 10^6 \text{ km}).

Worked example 2

The red giant star Betelgeuse has a surface temperature of approximately 3500 K and a luminosity of 5.0×10315.0 \times 10^{31} W. The Sun has a surface temperature of 5800 K and a luminosity of 3.8×10263.8 \times 10^{26} W. Calculate the ratio of Betelgeuse's radius to the Sun's radius (rB/rSr_B / r_S).

Show solution outline
  1. State the Stefan-Boltzmann Law for both stars: For Betelgeuse (B): LB=4πrB2σTB4L_B = 4\pi r_B^2 \sigma T_B^4 For the Sun (S): LS=4πrS2σTS4L_S = 4\pi r_S^2 \sigma T_S^4

  2. Create a ratio of the two equations to eliminate constants: Divide the equation for Betelgeuse by the equation for the Sun: LBLS=4πrB2σTB44πrS2σTS4\frac{L_B}{L_S} = \frac{4\pi r_B^2 \sigma T_B^4}{4\pi r_S^2 \sigma T_S^4} The constants 4π4\pi and σ\sigma cancel out: LBLS=rB2TB4rS2TS4=(rBrS)2(TBTS)4\frac{L_B}{L_S} = \frac{r_B^2 T_B^4}{r_S^2 T_S^4} = (\frac{r_B}{r_S})^2 (\frac{T_B}{T_S})^4

  3. Rearrange the formula to solve for the radius ratio (rB/rSr_B/r_S): (rBrS)2=LBLS×(TSTB)4(\frac{r_B}{r_S})^2 = \frac{L_B}{L_S} \times (\frac{T_S}{T_B})^4 rBrS=LBLS×(TSTB)4\frac{r_B}{r_S} = \sqrt{\frac{L_B}{L_S} \times (\frac{T_S}{T_B})^4}

  4. Substitute the given values and calculate: Luminosity ratio: LBLS=5.0×1031 W3.8×1026 W=1.316×105\frac{L_B}{L_S} = \frac{5.0 \times 10^{31} \text{ W}}{3.8 \times 10^{26} \text{ W}} = 1.316 \times 10^5 Temperature ratio: TSTB=5800 K3500 K=1.657\frac{T_S}{T_B} = \frac{5800 \text{ K}}{3500 \text{ K}} = 1.657

    Now substitute these into the rearranged formula: rBrS=(1.316×105)×(1.657)4\frac{r_B}{r_S} = \sqrt{(1.316 \times 10^5) \times (1.657)^4} rBrS=(1.316×105)×7.553\frac{r_B}{r_S} = \sqrt{(1.316 \times 10^5) \times 7.553} rBrS=9.936×105\frac{r_B}{r_S} = \sqrt{9.936 \times 10^5} rBrS=996.8\frac{r_B}{r_S} = 996.8

Betelgeuse's radius is approximately 997 times larger than the Sun's radius. This demonstrates why it is classified as a supergiant: it is extremely large to be so luminous despite its relatively cool surface temperature.